Critical properties of the valence-bond-solid transition in lattice quantum electrodynamics
arXiv:2003.09226 · doi:10.1103/PhysRevD.101.094505
Abstract
Elucidating the phase diagram of lattice gauge theories with fermionic matter in 2+1 dimensions has become a problem of considerable interest in recent years, motivated by physical problems ranging from chiral symmetry breaking in high-energy physics to fractionalized phases of strongly correlated materials in condensed matter physics. For a sufficiently large number of flavors of four-component Dirac fermions, recent sign-problem-free quantum Monte Carlo studies of lattice quantum electrodynamics (QED) on the square lattice have found evidence for a continuous quantum phase transition between a power-law correlated conformal QED phase and a confining valence-bond-solid phase with spontaneously broken point-group symmetries. The critical continuum theory of this transition was shown to be the QED-Gross-Neveu model, equivalent to the gauged Nambu-Jona-Lasinio model, and critical exponents were computed to first order in the large- expansion and the expansion. We extend these studies by computing critical exponents to second order in the large- expansion and to four-loop order in the expansion below four spacetime dimensions. In the latter context, we also explicitly demonstrate that the discrete symmetry of the valence-bond-solid order parameter is dynamically enlarged to a continuous symmetry at criticality for all values of .
arXiv comment16 pages, 6 figures, 8 tables; v2: published version
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